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  "body": "\n## Definition\n\nLet $(X, \\Sigma, \\mu)$ be a [[measure space|P15VQS5DJ9]].\nLet $f \\colon X \\to \\R$ or $f \\colon X \\to \\C$ be a [[measurable function|YYNCJSR0PJ]].\nThe function $f$ is *integrable*, or *Lebesgue integrable*, if\n$$\\int_X \\abs{f} \\, d\\mu \u003c \\infty,$$\nwhere the left side is the [[integral of the non-negative function|DG76G5Z6XW]] $\\abs{f}$.\n\n## Remarks\n\nExample: on $\\R$ with Lebesgue measure, $f(x) = e^{-\\abs{x}}$ is measurable since it is continuous.\nIts integral is $\\int_\\R e^{-\\abs{x}} \\, dx = 2 \u003c \\infty$, so $f$ is integrable.\n\nNon-example: $g(x) = \\sin(x) / x$ on $[1, \\infty)$ with Lebesgue measure is measurable but not integrable.\nOn each interval $[k\\pi, (k+1)\\pi]$ the integral of $\\abs{g}$ is at least $2 / ((k+1)\\pi)$, and these bounds have an infinite sum.\nIts improper Riemann integral still converges, so improper integrals and Lebesgue integrals differ here.\n\nA real function $f$ is integrable if and only if both $f^+ = \\max(f, 0)$ and $f^- = \\max(-f, 0)$ have finite integral.\nA function with values in $[-\\infty, \\infty]$ is called integrable under the same condition, and it is then finite almost everywhere.\nThe integrable functions form a vector space, often written $\\mathcal{L}^1(\\mu)$.\n",
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